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1.
In this paper, a higher order p-Laplacian neutral functional differential equation with a deviating argument:
[φp([x(t)−c(t)x(tσ)](n))](m)+f(x(t))x(t)+g(t,x(tτ(t)))=e(t)  相似文献   

2.
A multiplicity result for the singular ordinary differential equation y+λx−2yσ=0, posed in the interval (0,1), with the boundary conditions y(0)=0 and y(1)=γ, where σ>1, λ>0 and γ?0 are real parameters, is presented. Using a logarithmic transformation and an integral equation method, we show that there exists Σ?∈(0,σ/2] such that a solution to the above problem is possible if and only if λγσ−1?Σ?. For 0<λγσ−1<Σ?, there are multiple positive solutions, while if γ=(λ−1Σ?)1/(σ−1) the problem has a unique positive solution which is monotonic increasing. The asymptotic behavior of y(x) as x0+ is also given, which allows us to establish the absence of positive solution to the singular Dirichlet elliptic problem −Δu=d−2(x)uσ in Ω, where ΩRN, N?2, is a smooth bounded domain and d(x)=dist(x,∂Ω).  相似文献   

3.
One-dimensional perturbed neutral delay differential equations of the form (x(t)−P(t,x(tτ)))′=f(t,xt)+g(t,xt) are considered assuming that f satisfies −v(t)M(φ)?f(t,φ)?v(t)M(−φ), where M(φ)=max{0,maxs∈[−r,0]φ(s)}. A typical result is the following: if ‖g(t,φ)‖?w(t)‖φ‖ and , then the zero solution is uniformly asymptotically stable providing that the zero solution of the corresponding equation without perturbation (x(t)−P(t,x(tτ)))′=f(t,xt) is uniformly asymptotically stable. Some known results associated with this equation are extended and improved.  相似文献   

4.
Let X={X(s)}sS be an almost sure continuous stochastic process (S compact subset of Rd) in the domain of attraction of some max-stable process, with index function constant over S. We study the tail distribution of ∫SX(s)ds, which turns out to be of Generalized Pareto type with an extra ‘spatial’ parameter (the areal coefficient from Coles and Tawn (1996) [3]). Moreover, we discuss how to estimate the tail probability P(∫SX(s)ds>x) for some high value x, based on independent and identically distributed copies of X. In the course we also give an estimator for the areal coefficient. We prove consistency of the proposed estimators. Our methods are applied to the total rainfall in the North Holland area; i.e. X represents in this case the rainfall over the region for which we have observations, and its integral amounts to total rainfall.The paper has two main purposes: first to formalize and justify the results of Coles and Tawn (1996) [3]; further we treat the problem in a non-parametric way as opposed to their fully parametric methods.  相似文献   

5.
6.
The aim of this paper is to establish several necessary and sufficient conditions in order that the weighted inequality ρ(M f > λ)Φ(λ) ≤ C ∫_Ω~Ψ (C|f|)σdμ,λ > 0 or ρ(Mf>λ) ≤ C∫-Ω~Φ(Cλ~-1 |f|)σdμ,λ >0 holds for every uniformly integral martingale f=(f_n), where M is the Doob’s maximal operator, Φ, Ψ are both Φ-functions, and e, σ are weights.  相似文献   

7.
We study the Cauchy problem for the nonlinear heat equation ut-?u=|u|p-1u in RN. The initial data is of the form u0=λ?, where ?C0(RN) is fixed and λ>0. We first take 1<p<pf, where pf is the Fujita critical exponent, and ?C0(RN)∩L1(RN) with nonzero mean. We show that u(t) blows up for λ small, extending the H. Fujita blowup result for sign-changing solutions. Next, we consider 1<p<ps, where ps is the Sobolev critical exponent, and ?(x) decaying as |x|-σ at infinity, where p<1+2/σ. We also prove that u(t) blows up when λ is small, extending a result of T. Lee and W. Ni. For both cases, the solution enjoys some stable blowup properties. For example, there is single point blowup even if ? is not radial.  相似文献   

8.
In this paper, we derive an explicit expression for the parameter sequences of a chain sequence in terms of the corresponding orthogonal polynomials and their associated polynomials. We use this to study the orthogonal polynomials Kn(λ,M,k) associated with the probability measure dφ(λ,M,k;x), which is the Gegenbauer measure of parameter λ+1 with two additional mass points at ±k. When k=1 we obtain information on the polynomials Kn(λ,M) which are the symmetric Koornwinder polynomials. Monotonicity properties of the zeros of Kn(λ,M,k) in relation to M and k are also given.  相似文献   

9.
The instability property of the standing wave uω(t, x) = eiωtφ(x) for the Klein–Gordon– Hartree equation  相似文献   

10.
Let C be a convex body, and let S be a nondegenerate simplex in ? n . It is proved that the minimal coefficientσ > 0 for which the translate of σS contains C is $$\sum\limits_{j = 1}^{n + 1} {\mathop {\max \left( { - \lambda _j \left( x \right)} \right) + 1,}\limits_{x \in C} }$$ where λ 1(x), ..., λ n +1(x) are the barycentric coordinates of the point x ∈ ? n with respect to S. In the case C = [0, 1] n , this quantity is reduced to the form Σ i=1 n 1/d i (S), where d i (S) is the ith axial diameter of S, i.e., the maximal length of the segment from S parallel to the ith coordinate axis.  相似文献   

11.
In this paper we consider a new integrable equation (the Degasperis-Procesi equation) derived recently by Degasperis and Procesi (1999) [3]. Analogous to the Camassa-Holm equation, this new equation admits blow-up phenomenon and infinite propagation speed. First, we give a proof for the blow-up criterion established by Zhou (2004) in [12]. Then, infinite propagation speed for the Degasperis-Procesi equation is proved in the following sense: the corresponding solution u(x,t) with compactly supported initial datum u0(x) does not have compact x-support any longer in its lifespan. Moreover, we show that for any fixed time t>0 in its lifespan, the corresponding solution u(x,t) behaves as: u(x,t)=L(t)ex for x?1, and u(x,t)=l(t)ex for x?−1, with a strictly increasing function L(t)>0 and a strictly decreasing function l(t)<0 respectively.  相似文献   

12.
Let K be a compact subset of Rd and let m define a semi-dynamical system on M1(K),, the space of probability measures on K, induced by a homogeneous Markov process. Let J(φ) be the prolongational limit set for φ?M1(K). The main result of the paper is the decomposition: support of J(φ) = ∪ {support of J(δx): x? support φ}, where δx is the Dirac measure at the point x.  相似文献   

13.
We give some properties relating the recurrence relations of orthogonal polynomials associated with any two symmetric distributions dφ1(x) and d2(x) such that dφ2(x) = (1 + kx2)d1(x). As applications of properties, recurrence relations for many interesting systems of orthogonal polynomials are obtained.  相似文献   

14.
Let be a contractive gauge function in the sense that φ is continuous, φ(s)<s for s>0, and if f:M→M satisfies d(f(x),f(y))?φ(d(x,y)) for all x,y in a complete metric space (M,d), then f always has a unique fixed point. It is proved that if T:M→M satisfies
  相似文献   

15.
By using the theory of coincidence degree, we study a kind of periodic solutions to p-Laplacian neutral functional differential equation with deviating arguments such as (φp(x(t)−cx(tσ)))+g(t,x(tτ(t)))=p(t), a result on the existence of periodic solutions is obtained.  相似文献   

16.
The paper studies the blowup of solutions to the initial boundary value problem for the “bad” Boussinesq-type equation uttuxxbuxxxx=σ(u)xx, where b>0 is a real number and σ(s) is a given nonlinear function. By virtue of the energy method and the Fourier transform method, respectively, it proves that under certain assumptions on σ(s) and initial data, the generalized solutions of the above-mentioned problem blow up in finite time. And a few examples are shown, especially for the “bad” Boussinesq equation, two examples of blowup of solutions are obtained numerically.  相似文献   

17.
Let IR be a non-trivial interval and let . We present some results concerning the following functional equation, generalizing the Matkowski-Sutô equation,
λ(x,y)φ−1(μ(x,y)φ(x)+(1−μ(x,y))φ(y))+(1−λ(x,y))ψ−1(ν(x,y)ψ(x)+(1−ν(x,y))ψ(y))=λ(x,y)x+(1−λ(x,y))y,  相似文献   

18.
If the potential in a three-particle system is the boundary value of an analytic function, the physical Hamiltonian H(0) has a dilation-analytic continuation H(φ). The continuous spectrum of H(φ) consists of half-lines Y(λp, φ) starting at the thresholds λp of scattering channels and making angles 2φ with the positive real axis. If the interaction is the sum of local two-body potentials in suitable Lp-spaces, each half-line Y(λp, φ) is associated with an operator P(λp, φ) that projects onto an invariant subspace of H(φ). Suppose Y(λp, φ) does not pass through any two- or three-particle eigenvalues λλp when φ runs through some interval 0 < α ? φ ? β < π2. For φ in [α, β], this paper shows that the resolvent R(λ, φ) has smoothness properties near Y(λp, φ) that are sufficient for P(λp, φ)[H(φ) ? λp] e?2 to be spectral and to generate a strongly differentiable group. The projection, the group, and the spectral resolution operators are norm continuous in φ. These results are not affected by any spurious poles of the resolvent equation. At a spurious pole λ = λp + ze2, the resolvent R(λp + ze2,φ) is examined by a method that uses two resolvent equations in succession and shows that there is norm continuity in z, φ. The case of spurious poles on Y(λp, φ) is included.  相似文献   

19.
Let A and B be invertible positive elements in a II1-factor A, and let μs(·) be the singular number on A. We prove that
expKlogμs(AB)ds?expIlogμs(A)ds·expJlogμs(B)ds,  相似文献   

20.
In the case of oscillatory potentials, we establish an oscillation theorem for the forced sublinear differential equation x(n)+q(t)λ|x|sgnx=e(t), t∈[t0,∞). No restriction is imposed on the forcing term e(t) to be the nth derivative of an oscillatory function. In particular, we show that all solutions of the equation x+tαsintλ|x|sgnx=mtβcost, t?0, 0<λ<1 are oscillatory for all m≠0 if β>(α+2)/(1−λ). This provides an analogue of a result of Nasr [Proc. Amer. Math. Soc. 126 (1998) 123] for the forced superlinear equation and answers a question raised in an earlier paper [J.S.W. Wong, SIAM J. Math. Anal. 19 (1988) 673].  相似文献   

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